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geant4/source/geometry/magneticfield/include/G4ClassicalRK4.hh
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2016-06-08 16:57:27 +02:00

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// $Id: G4ClassicalRK4.hh,v 1.6 2002/11/20 17:56:35 japost Exp $
// GEANT4 tag $Name: geant4-05-00 $
//
//
// class G4ClassicalRK4
//
// Class description:
//
// Integrate the equations of the motion of a particle in a magnetic field
// using the classical 4th Runge-Kutta method.
// History:
// - Created: J.Apostolakis, V.Grichine - 30.1.97
// - Moved into G4MagErrorStepper: W.Wander <wwc@mit.edu> - 12/09/97
#include "G4MagErrorStepper.hh"
#include "G4ThreeVector.hh"
class G4ClassicalRK4 : public G4MagErrorStepper
{
public: // with description
G4ClassicalRK4(G4Mag_EqRhs *EqRhs, G4int numberOfVariables = 6) ;
~G4ClassicalRK4() ;
// A stepper that does not know about errors.
// It is used by the MagErrorStepper stepper.
void DumbStepper( const G4double yIn[],
const G4double dydx[],
G4double h,
G4double yOut[]) ;
// Given values for the variables y[0,..,n-1] and their derivatives
// dydx[0,...,n-1] known at x, use the classical 4th Runge-Kutta
// method to advance the solution over an interval h and return the
// incremented variables as yout[0,...,n-1], which not be a distinct
// array from y. The user supplies the routine RightHandSide(x,y,dydx),
// which returns derivatives dydx at x. The source is routine rk4 from
// NRC p. 712-713 .
public: // without description
void StepWithEst( const G4double yIn[],
const G4double dydx[],
G4double h,
G4double yOut[],
G4double& alpha2,
G4double& beta2,
const G4double B1[],
G4double B2[] );
// Could make above G4SixPoint to keep tangents too ...?
G4int IntegratorOrder() const { return 4; }
private:
G4ClassicalRK4(const G4ClassicalRK4&);
G4ClassicalRK4& operator=(const G4ClassicalRK4&);
// Private copy constructor and assignment operator.
private:
// G4int fNumberOfVariables ; // is set default to 6 in constructor
G4double *dydxm, *dydxt, *yt; // scratch space - not state
};